Camera optical lens

ABSTRACT

The present disclosure relates to the field of optical lenses and provides a camera optical lens. The camera optical lens includes, from an object side to an image side: an aperture; a first lens having a positive refractive power; a second lens having a positive refractive power; a third lens having a negative refractive power; a fourth lens having a negative refractive power; a fifth lens having a positive refractive power; and a sixth lens having a negative refractive power. The camera optical lens satisfies following conditions: 8.00≤d1/d2≤12.00; and 2.80≤v1/v3≤4.00, where d1 denotes an on-axis thickness of the first lens; d2 denotes an on-axis distance from an image side surface of the first lens to an object side surface of the second lens; v1 denotes an abbe number of the first lens; and v3 denotes an abbe number of the third lens.

TECHNICAL FIELD

The present disclosure relates to the field of optical lens, and moreparticularly, to a camera optical lens suitable for handheld terminaldevices such as smart phones or digital cameras and camera devices suchas monitors or PC lenses.

BACKGROUND

With the emergence of smart phones in recent years, the demand forminiature camera lens is increasing day by day, but in general thephotosensitive devices of camera lens are nothing more than ChargeCoupled Device (CCD) or Complementary Metal-Oxide Semiconductor Sensor(CMOS sensor), and as the progress of the semiconductor manufacturingtechnology makes the pixel size of the photosensitive devices becomesmaller, plus the current development trend of electronic productstowards better functions and thinner and smaller dimensions, miniaturecamera lenses with good imaging quality therefore have become amainstream in the market.

In order to obtain better imaging quality, the lens that istraditionally equipped in mobile phone cameras adopts a three-piece orfour-piece lens structure, or even a five-piece structure. Also, withthe development of technology and the increase of the diverse demands ofusers, and as the pixel area of photosensitive devices is becomingsmaller and smaller and the requirement of the system on the imagingquality is improving constantly, a six-piece lens structure graduallyappears in lens designs. Although the common six-piece lens has goodoptical performance, its settings on refractive power, lens spacing andlens shape still have some irrationality, which results in that the lensstructure cannot achieve a high optical performance while satisfyingdesign requirements for ultra-thin lenses.

BRIEF DESCRIPTION OF DRAWINGS

Many aspects of the exemplary embodiment can be better understood withreference to the following drawings. The components in the drawings arenot necessarily drawn to scale, the emphasis instead being placed uponclearly illustrating the principles of the present disclosure. Moreover,in the drawings, like reference numerals designate corresponding partsthroughout the several views.

FIG. 1 is a schematic diagram of a structure of a camera optical lens inaccordance with Embodiment 1 of the present disclosure;

FIG. 2 is a schematic diagram of a longitudinal aberration of the cameraoptical lens shown in FIG. 1;

FIG. 3 is a schematic diagram of a lateral color of the camera opticallens shown in FIG. 1;

FIG. 4 is a schematic diagram of a field curvature and a distortion ofthe camera optical lens shown in FIG. 1;

FIG. 5 is a schematic diagram of a structure of a camera optical lens inaccordance with Embodiment 2 of the present disclosure;

FIG. 6 is a schematic diagram of a longitudinal aberration of the cameraoptical lens shown in FIG. 5;

FIG. 7 is a schematic diagram of a lateral color of the camera opticallens shown in

FIG. 5;

FIG. 8 is a schematic diagram of a field curvature and a distortion ofthe camera optical lens shown in FIG. 5;

FIG. 9 is a schematic diagram of a structure of a camera optical lens inaccordance with Embodiment 3 of the present disclosure;

FIG. 10 is a schematic diagram of a longitudinal aberration of thecamera optical lens shown in FIG. 9;

FIG. 11 is a schematic diagram of a lateral color of the camera opticallens shown in FIG. 9;

FIG. 12 is a schematic diagram of a field curvature and a distortion ofthe camera optical lens shown in FIG. 9;

FIG. 13 is a schematic diagram of a structure of a camera optical lensin accordance with Embodiment 4 of the present disclosure;

FIG. 14 is a schematic diagram of a longitudinal aberration of thecamera optical lens shown in FIG. 13;

FIG. 15 is a schematic diagram of a lateral color of the camera opticallens shown in FIG. 13; and

FIG. 16 is a schematic diagram of a field curvature and a distortion ofthe camera optical lens shown in FIG. 13.

DESCRIPTION OF EMBODIMENTS

The present disclosure will hereinafter be described in detail withreference to several exemplary embodiments. To make the technicalproblems to be solved, technical solutions and beneficial effects of thepresent disclosure more apparent, the present disclosure is described infurther detail together with the figure and the embodiments. It shouldbe understood the specific embodiments described hereby is only toexplain the disclosure, not intended to limit the disclosure.

Embodiment 1

Referring to FIG. 1, the present disclosure provides a camera opticallens 10. FIG. 1 shows the camera optical lens 10 according to Embodiment1 of the present disclosure. The camera optical lens 10 includes 6lenses. Specifically, the camera optical lens 10 includes, from anobject side to an image side, an aperture S1, a first lens L1, a secondlens L2, a third lens L3, a fourth lens L4, a fifth lens L5 and a sixthlens L6. An optical element such as a glass plate GF can be arrangedbetween the sixth lens L6 and an image plane Si. The glass plate GF canbe a glass cover plate or an optical filter. In other embodiments, theglass plate GF can be arranged at other position.

In present embodiment, the first lens L1 has a positive refractivepower, and has an object side surface being a convex surface and animage object surface being a concave surface; the second lens L2 has apositive refractive power, and has an object side surface being a convexsurface and an image object surface being a concave surface; the thirdlens L3 has a negative refractive power, and has an object side surfacebeing a concave surface and an image object surface being a concavesurface; the fourth lens L4 has a negative refractive power, and has anobject side surface being a convex surface and an image object surfacebeing a concave surface; the fifth lens L5 has a positive refractivepower, and has an object side surface being a convex surface and animage object surface being a convex surface; and a sixth lens L6 has anegative refractive power, and has an object side surface being aconcave surface and an image object surface being a convex surface.

Here, an on-axis thickness of the first lens is defined as d1, anon-axis distance from the image side surface of the first lens to theobject side surface of the second lens is defined as d2, an abbe numberof the first lens is defined as v1, and an abbe number of the third lensis defined as v3. The camera optical lens 10 should satisfy followingconditions:

8.00≤d1/d2≤12.00  (1); and

2.80≤v1/v3≤4.00  (2).

The condition (1) specifies a ratio of the on-axis thickness d1 of thefirst lens L1 and the on-axis distance d2 from the image side surface ofthe first lens L1 to the object side surface of the second lens L2. Thiscan facilitate processing and assembly of the lenses.

The condition (2) specifies a ratio of the abbe number v1 of the firstlens L1 and the abbe number v3 of the third lens L3. This can facilitatereducing a total length of the camera optical lens, achieving ultra-thinlenses, correction of aberrations and improving the imaging performance.

In this embodiment, with the above configurations of the lenses, thecamera optical lens can achieve a high optical performance whilesatisfying design requirements for ultra-thin lenses.

In an example, a focal length of the first lens is defined as f1, and afocal length of the fifth lens is defined as f5. The camera optical lens10 should satisfy a following condition:

3.00≤f5/f1≤5.00  (3).

The condition (3) specifies a ratio of the focal length f5 of the fifthlens L5 and the focal length f1 of the first lens L1. This leads to theappropriate distribution of the refractive power for the first lens L1and the fifth lens L5, thereby facilitating improving the image qualityof the camera optical lens.

In an example, a curvature radius of the object side surface of thesecond lens is defined R3, and a curvature radius of the image sidesurface of the second lens is defined as R4. The camera optical lens 10should satisfy a following condition:

−5.00≤(R3+R4)/(R3−R4)≤−1.00  (4).

The condition (4) specifies a shape of the second lens L2. This canalleviate a deflection degree of light passing through the lens, therebyeffectively reducing aberrations.

In an example, a focal length of the camera optical lens is defined asf, and a focal length of the first lens is defined as f1. The cameraoptical lens 10 should satisfy a following condition:

0.50≤f1/f≤0.80  (5).

The condition (5) specifies a ratio of the focal length f1 of the firstlens L1 and the focal length f of the camera optical lens. This leads tothe appropriate distribution of the refractive power for the first lens,thereby facilitating correction of aberrations while improving theimaging quality of the camera optical lens.

In an example, a curvature radius of the object side surface of thefourth lens is defined as R7, and a curvature radius of the image sidesurface of the fourth lens is defined as R8. The camera optical lens 10should satisfy a following condition:

1.00≤(R7+R8)/(R7−R8)≤3.00  (6).

The condition (6) specifies a shape of the fourth lens L4. This caneffectively correct aberrations caused by the first three lenses (L1, L2and L3) of the camera optical lens.

In addition, a surface of a lens can be set as an aspherical surface.The aspherical surface can be easily formed into a shape other than thespherical surface, so that more control variables can be obtained toreduce the aberration, thereby reducing the number of lenses and thuseffectively reducing a total length of the camera optical lens accordingto the present disclosure. In an embodiment of the present disclosure,both an object side surface and an image side surface of each lens areaspherical surfaces.

It should be noted that the first lens L1, the second lens L2, the thirdlens L3, the fourth lens L4, the fifth lens L5 and the sixth lens L6that constitute the camera optical lens 10 of the present embodimenthave the structure and parameter relationships as described above, andtherefore, the camera optical lens 10 can reasonably distribute therefractive power, the surface shape, the on-axis thickness and the likeof each lens, and thus correct various aberrations. A total opticallength from the object side surface of the first lens to an image planeof the camera optical lens along an optic axis (TTL) and the focallength f of the camera optical lens 10 satisfy a condition ofTTL/f≤0.89. This can achieve a high imaging performance while satisfyingdesign requirements for ultra-thin lenses.

In an example, inflexion points and/or arrest points can be arranged onthe object side surface and/or image side surface of the lens, so as tosatisfy the demand for the high quality imaging. The description belowcan be referred to for specific implementations.

The design information of the camera optical lens 10 in Embodiment 1 ofthe present disclosure is shown in the following. It should be notedthat each of the distance, radii and the central thickness is in a unitof millimeter (mm).

Table 1 and Table 2 show design data of the camera optical lens 10according to Embodiment 1 of the present disclosure.

TABLE 1 R d nd νd S1 ∞ d0= −0.556 R1 1.531 d1= 0.577 nd1 1.5264 ν1 76.86R2 5.184 d2= 0.055 R3 3.603 d3= 0.556 nd2 1.5444 ν2 55.82 R4 8.162 d4=0.123 R5 −13.330 d5= 0.230 nd3 1.6610 ν3 20.53 R6 6.389 d6= 0.264 R79.968 d7= 0.230 nd4 1.5444 ν4 55.82 R8 2.501 d8= 0.770 R9 63.707 d9=0.335 nd5 1.6610 ν5 20.53 R10 −12.167 d10= 1.219 R11 −3.076 d11= 0.609nd6 1.5346 ν6 55.69 R12 −10.766 d12= 0.392 R13 ∞ d13= 0.200 ndg 1.5168νg 64.17 R14 ∞ d14= 0.125

In the table, meanings of various symbols will be described as follows.

S1: aperture;

R: curvature radius of an optical surface, a central curvature radiusfor a lens;

R1: curvature radius of the object side surface of the first lens L1;

R2: curvature radius of the image side surface of the first lens L1;

R3: curvature radius of the object side surface of the second lens L2;

R4: curvature radius of the image side surface of the second lens L2;

R5: curvature radius of the object side surface of the third lens L3;

R6: curvature radius of the image side surface of the third lens L3;

R7: curvature radius of the object side surface of the fourth lens L4;

R8: curvature radius of the image side surface of the fourth lens L4;

R9: curvature radius of the object side surface of the fifth lens L5;

R10: curvature radius of the image side surface of the fifth lens L5;

R11: curvature radius of the object side surface of the sixth lens L6;

R12: curvature radius of the image side surface of the sixth lens L6;

R13: curvature radius of an object side surface of the optical filterGF;

R14: curvature radius of an image side surface of the optical filter GF;

d: on-axis thickness of a lens or an on-axis distance between lenses;

d0: on-axis distance from the aperture S1 to the object side surface ofthe first lens L1;

d1: on-axis thickness of the first lens L1;

d2: on-axis distance from the image side surface of the first lens L1 tothe object side surface of the second lens L2;

d3: on-axis thickness of the second lens L2;

d4: on-axis distance from the image side surface of the second lens L2to the object side surface of the third lens L3;

d5: on-axis thickness of the third lens L3;

d6: on-axis distance from the image side surface of the third lens L3 tothe object side surface of the fourth lens L4;

d7: on-axis thickness of the fourth lens L4;

d8: on-axis distance from the image side surface of the fourth lens L4to the object side surface of the fifth lens L5;

d9: on-axis thickness of the fifth lens L5;

d10: on-axis distance from the image side surface of the fifth lens L5to the object side surface of the sixth lens L6;

d11: on-axis thickness of the sixth lens L6;

d12: on-axis distance from the image side surface of the sixth lens L6to the object side surface of the optical filter GF;

d13: on-axis thickness of the optical filter GF;

d14: on-axis distance from the image side surface of the optical filterGF to the image plane Si;

nd: refractive index of d line;

nd1: refractive index of d line of the first lens L1;

nd2: refractive index of d line of the second lens L2;

nd3: refractive index of d line of the third lens L3;

nd4: refractive index of d line of the fourth lens L4;

nd5: refractive index of d line of the fifth lens L5;

nd6: refractive index of d line of the sixth lens L6;

ndg: refractive index of d line of the optical filter GF;

vd: abbe number;

v1: abbe number of the first lens L1;

v2: abbe number of the second lens L2;

v3: abbe number of the third lens L3;

v4: abbe number of the fourth lens L4;

v5: abbe number of the fifth lens L5;

v6: abbe number of the sixth lens L6;

vg: abbe number of the optical filter GF.

Table 2 shows aspheric surface data of respective lens in the cameraoptical lens 10 according to Embodiment 1 of the present disclosure.

TABLE 2 Conic coefficient Aspherical surface coefficients k A4 A6 A8 A10A12 A14 A16 R1 −5.0781E−01  2.1486E−04 1.4677E−02 −1.3472E−02  8.8067E−03  1.8782E−03 −1.0885E−03 −9.9610E−04  R2  2.4517E+00 1.4649E−02 5.7226E−02 2.2471E−02 −5.0488E−03 −1.3003E−02 −1.4693E−028.1742E−03 R3  4.3207E+00  2.9515E−02 8.0031E−02 1.0147E−02 −8.2861E−03−1.1337E−02 −1.1203E−02 4.0379E−03 R4  2.4234E+01 −2.1144E−02−2.2113E−02  1.9843E−02 −8.6229E−03 −1.9406E−02  2.2770E−02 −8.2509E−03 R5 −4.8214E+02 −1.1763E−02 1.0151E−01 −6.7230E−02   2.0588E−02 9.8419E−02 −1.3970E−01 6.5557E−02 R6 −4.6000E+02  1.8008E−01−1.4266E−01  2.5494E−01  4.7342E−01 −8.8335E−01  3.5832E−01 2.6149E−01R7  8.9551E+01 −3.2692E−01 1.1015E−01 4.1641E−01 −7.7895E−01 −1.1348E−01 1.2963E+00 −1.1012E+00  R8 −1.7579E+01 −1.0864E−01 1.5219E−01−2.6652E−02  −6.2423E−02 −1.3714E−02  1.0825E−04 2.2444E−02 R9 8.9625E+01 −5.5395E−02 −4.4782E−03  2.3626E−02 −4.6383E−03 −1.8770E−03 8.7557E−04 −1.8434E−04  R10 −1.6297E+01 −5.2100E−02 5.3599E−033.3305E−03  2.1914E−03  9.1920E−05 −3.4607E−04 3.0756E−06 R11−1.6082E−01 −6.9184E−02 2.7189E−02 −4.0178E−03  −2.7485E−04  3.4958E−04−5.9541E−05 2.6755E−06 R12 −8.5036E+00 −1.1705E−01 4.2940E−02−1.0459E−02   9.8146E−04  2.2398E−04 −8.2659E−05 7.8517E−06

Herein, k is a conic coefficient, and A4, A6, A8, A10, A12, A14 and A16are aspheric surface coefficients.

IH: Image Height

y=(x ² /R)/[1+{1−(k+1)(x ² R ²)}^(1/2)]+A4x ⁴ +A6x ⁶ +A8x ⁸ +A10x ¹⁰+A12x ¹² +A14x ¹⁴ +A16x ¹⁶  (7)

In the present embodiment, an aspheric surface of each lens surface usesthe aspheric surfaces shown in the above condition (7). However, thepresent disclosure is not limited to the aspherical polynomials formshown in the condition (7).

Table 3 and Table 4 show design data of inflexion points and arrestpoints of respective lens in the camera optical lens 10 according toEmbodiment 1 of the present disclosure. P1R1 and P1R2 represent theobject side surface and the image side surface of the first lens L1,respectively, P2R1 and P2R2 represent the object side surface and theimage side surface of the second lens L2, respectively, P3R1 and P3R2represent the object side surface and the image side surface of thethird lens L3, respectively, P4R1 and P4R2 represent the object sidesurface and the image side surface of the fourth lens L4, respectively,P5R1 and P5R2 represent the object side surface and the image sidesurface of the fifth lens L5, respectively, and P6R1 and P6R2 representthe object side surface and the image side surface of the sixth lens L6,respectively. The data in the column named “inflexion point position”refers to vertical distances from inflexion points arranged on each lenssurface to the optic axis of the camera optical lens 10. The data in thecolumn named “arrest point position” refers to vertical distances fromarrest points arranged on each lens surface to the optic axis of thecamera optical lens 10.

TABLE 3 Number of Inflexion point Inflexion point Inflexion pointinflexion points position 1 position 2 position 3 P1R1 1 1.205 P1R2 11.045 P2R1 1 1.035 P2R2 1 0.615 P3R1 1 0.405 P3R2 P4R1 1 0.175 P4R2 10.745 P5R1 3 0.155 1.015 1.315 P5R2 2 1.105 1.465 P6R1 1 1.485 P6R2 12.035

TABLE 4 Number of Arrest point arrest points position 1 P1R1 P1R2 P2R1P2R2 1 0.935 P3R1 1 0.625 P3R2 P4R1 1 0.295 P4R2 P5R1 1 0.265 P5R2 P6R1P6R2

FIG. 2 and FIG. 3 illustrate a longitudinal aberration and a lateralcolor of light with wavelengths of 470 nm, 510 nm, 555 nm, 610 nm and650 nm after passing the camera optical lens 10 according toEmbodiment 1. FIG. 4 illustrates a field curvature and a distortion oflight with a wavelength of 555 nm after passing the camera optical lens10 according to Embodiment 1, in which a field curvature S is a fieldcurvature in a sagittal direction and T is a field curvature in atangential direction.

Table 17 below further lists various values of Embodiments 1, 2, 3 and 4and values corresponding to parameters which are specified in the aboveconditions.

As shown in Table 17, Embodiment 1 satisfies respective conditions.

In this embodiment, the entrance pupil diameter of the camera opticallens is 2.479 mm. The image height of 1.0H is 2.628 mm. The FOV (fieldof view) is 45.11°. Thus, the camera optical lens is ultra-thin whileachieving a high optical performance.

Embodiment 2

Embodiment 2 is basically the same as Embodiment 1 and involves symbolshaving the same meanings as Embodiment 1, and only differencestherebetween will be described in the following.

Table 5 and Table 6 show design data of a camera optical lens 20 inEmbodiment 2 of the present disclosure.

TABLE 5 R d nd νd S1 ∞ d0= −0.557 R1 1.520 d1= 0.584 nd1 1.4970 ν1 81.61R2 8.425 d2= 0.073 R3 4.693 d3= 0.595 nd2 1.5444 ν2 55.82 R4 7.256 d4=0.125 R5 −22.066 d5= 0.230 nd3 1.6610 ν3 20.53 R6 6.196 d6= 0.353 R7608.436 d7= 0.230 nd4 1.5444 ν4 55.82 R8 3.026 d8= 0.551 R9 18.717 d9=0.324 nd5 1.6610 ν5 20.53 R10 −12.727 d10= 1.330 R11 −2.834 d11= 0.573nd6 1.5346 ν6 55.69 R12 −9.399 d12= 0.392 R13 ∞ d13= 0.200 ndg 1.5168 νg64.17 R14 ∞ d14= 0.126

Table 6 shows aspheric surface data of respective lenses in the cameraoptical lens 20 according to Embodiment 2 of the present disclosure.

TABLE 6 Conic coefficient Aspherical surface coefficients k A4 A6 A8 A10A12 A14 A16 R1 −5.5890E−01 −1.9710E−03 1.3000E−02 −1.3777E−02  1.4130E−02  3.3771E−04 −2.1023E−03 −6.7396E−04  R2 −2.2736E+01 1.3278E−02 6.6551E−02 2.5837E−02  1.6685E−03 −1.1340E−02 −1.8721E−028.9448E−03 R3  7.0944E+00  2.7108E−02 8.7334E−02 2.8573E−02 −2.0355E−02−1.7339E−02  3.9062E−03 1.6154E−03 R4  2.0753E+00 −3.7846E−02−5.2689E−03  2.6995E−02 −5.7629E−03 −2.9949E−02  1.8516E−02 9.7306E−05R5  7.8520E+01 −5.0017E−02 1.3246E−01 −5.4306E−02  −1.7280E−02 8.6862E−02 −1.1775E−01 5.7268E−02 R6 −3.6705E+02  1.1815E−01−6.3036E−02  2.9416E−01  1.4533E−01 −1.0160E+00  1.5316E+00 −7.5827E−01 R7  9.9331E+00 −4.0528E−01 2.8528E−01 2.9508E−01 −9.5884E−01  2.9290E−02 1.9040E+00 −1.7904E+00  R8 −5.3733E+01 −1.3805E−01 1.3709E−01−2.7432E−03  −2.4657E−02 −1.7144E−02 −6.5860E−02 5.6152E−02 R9 8.9275E+01 −6.8248E−02 −4.9829E−03  2.9176E−02 −2.7476E−03 −3.3638E−03−3.5398E−04 3.4815E−04 R10 −3.1771E+01 −4.7467E−02 −1.6350E−03 8.5328E−03  2.7887E−03 −4.0351E−04 −5.2067E−04 4.6959E−05 R11−1.3620E−01 −6.3523E−02 2.9653E−02 −4.9816E−03  −3.7896E−04  3.8551E−04−4.7806E−05 3.5557E−07 R12 −6.5245E+00 −1.1238E−01 4.2440E−02−1.0477E−02   9.8683E−04  2.2409E−04 −8.4391E−05 8.2162E−06

Table 7 and Table 8 show design data of inflexion points and arrestpoints of respective lens in the camera optical lens 20 according toEmbodiment 2 of the present disclosure.

TABLE 7 Number of Inflexion point Inflexion point Inflexion pointinflexion points position 1 position 2 position 3 P1R1 1 1.195 P1R2 11.085 P2R1 P2R2 2 0.615 1.015 P3R1 1 0.505 P3R2 P4R1 1 0.025 P4R2 10.365 P5R1 3 0.265 0.955 1.275 P5R2 2 1.045 1.425 P6R1 1 1.495 P6R2 12.015

TABLE 8 Number of Arrest point arrest points position 1 P1R1 P1R2 P2R1P2R2 P3R1 1 0.705 P3R2 P4R1 1 0.035 P4R2 1 0.885 P5R1 1 0.455 P5R2 P6R1P6R2

FIG. 6 and FIG. 7 illustrate a longitudinal aberration and a lateralcolor of light with wavelengths of 470 nm, 510 nm, 555 nm, 610 nm and650 nm after passing the camera optical lens 20 according to Embodiment2. FIG. 8 illustrates a field curvature and a distortion of light with awavelength of 555 nm after passing the camera optical lens 20 accordingto Embodiment 2.

As shown in Table 17, Embodiment 2 satisfies respective conditions.

In this embodiment, the entrance pupil diameter of the camera opticallens is 2.479 mm. The image height of 1.0H is 2.628 mm. The FOV (fieldof view) is 45.11°. Thus, the camera optical lens is ultra-thin whileachieving a high optical performance.

Embodiment 3

Embodiment 3 is basically the same as Embodiment 1 and involves symbolshaving the same meanings as Embodiment 1, and only differencestherebetween will be described in the following.

Table 9 and Table 10 show design data of a camera optical lens 30 inEmbodiment 3 of the present disclosure.

TABLE 9 R d nd νd S1 ∞ d0= −0.532 R1 1.667 d1= 0.501 nd1 1.5831 ν1 59.38R2 11.373 d2= 0.062 R3 5.875 d3= 0.647 nd2 1.5444 ν2 55.82 R4 8.827 d4=0.104 R5 −10.950 d5= 0.230 nd3 1.6610 ν3 20.53 R6 6.737 d6= 0.247 R7164.784 d7= 0.230 nd4 1.5444 ν4 55.82 R8 4.053 d8= 1.273 R9 −7.292 d9=0.463 nd5 1.6610 ν5 20.53 R10 −4.466 d10= 0.731 R11 −2.527 d11= 0.478nd6 1.5346 ν6 55.69 R12 −9.616 d12= 0.392 R13 ∞ d13= 0.200 ndg 1.5168 νg64.17 R14 ∞ d14= 0.127

Table 10 shows aspheric surface data of respective lenses in the cameraoptical lens 30 according to Embodiment 3 of the present disclosure.

TABLE 10 Conic coefficient Aspherical surface coefficients k A4 A6 A8A10 A12 A14 A16 R1 −7.1581E−01 −1.4422E−02 5.2541E−02 −4.4947E−02 4.0386E−02 −3.8222E−03 −9.8095E−03 2.2113E−03 R2  8.2740E+01−1.5676E−02 1.8460E−01 −1.9257E−02 −1.2666E−02  6.9348E−03 −3.7460E−021.4691E−02 R3 −1.8567E+01  3.9552E−02 1.4291E−01  1.2013E−01 −1.5320E−01−6.0609E−02  1.2618E−01 −4.4371E−02  R4 −9.0022E+01 −1.6279E−011.9977E−01  4.8315E−02 −1.3522E−01 −5.2775E−02  1.0458E−01 −3.3008E−02 R5 −8.0821E+01 −1.1281E−01 3.9557E−01 −1.6843E−01 −1.9728E−01 1.6035E−01 −4.8726E−02 1.0887E−02 R6 −4.6001E+02  1.9224E−01 1.0134E−02 2.4312E−01  3.0386E−01 −2.2234E+00  3.8819E+00 −2.3887E+00  R7 8.9984E+01 −8.7625E−02 −2.0756E−01   1.1995E+00 −2.4937E+00  2.3274E+00−1.4995E−01 −9.7369E−01  R8 −4.0950E+01  2.0980E−02 4.8476E−02−2.0875E−01  6.3219E−01 −8.7349E−01  4.8579E−01 −8.1883E−02  R9 8.3354E+00 −2.2919E−02 −1.7050E−02   5.1475E−03 −3.0689E−03  7.6554E−04−4.2767E−05 7.5656E−05 R10 −3.1671E+01 −6.8832E−02 1.3403E−02−1.0071E−02  2.9568E−03 −1.6960E−04 −2.6894E−04 9.1872E−05 R11−5.2803E−01 −9.3346E−02 4.6082E−02 −7.0397E−03 −6.7829E−04  4.3397E−04−5.2808E−05 1.6581E−06 R12  5.0970E+00 −1.4018E−01 5.8151E−02−1.1610E−02  5.2355E−04  2.6586E−04 −6.5589E−05 5.1825E−06

Table 11 and Table 12 show design data of inflexion points and arrestpoints of respective lens in the camera optical lens 30 according toEmbodiment 3 of the present disclosure.

TABLE 11 Number of Inflexion point Inflexion point Inflexion pointinflexion points position 1 position 2 position 3 P1R1 1 1.195 P1R2 11.065 P2R1 1 1.105 P2R2 3 0.265 0.555 0.855 P3R1 2 0.435 0.845 P3R2 P4R11 0.075 P4R2 1 0.845 P5R1 1 1.415 P5R2 1 1.545 P6R1 1 1.465 P6R2 1 2.135

TABLE 12 Number of Arrest point Arrest point arrest points position 1position 2 P1R1 P1R2 P2R1 P2R2 1 0.965 P3R1 2 0.635 0.965 P3R2 P4R1 10.125 P4R2 P5R1 P5R2 P6R1 P6R2

FIG. 10 and FIG. 11 illustrate a longitudinal aberration and a lateralcolor of light with wavelengths of 470 nm, 510 nm, 555 nm, 610 nm and650 nm after passing the camera optical lens 30 according to Embodiment3. FIG. 12 illustrates field curvature and distortion of light with awavelength of 555 nm after passing the camera optical lens 30 accordingto Embodiment 3.

As shown in Table 17, Embodiment 3 satisfies respective conditions.

In this embodiment, the entrance pupil diameter of the camera opticallens is 2.479 mm. The image height of 1.0H is 2.629 mm. The FOV (fieldof view) is 45.11°. Thus, the camera optical lens is ultra-thin whileachieving a high optical performance.

Embodiment 4

Embodiment 4 is basically the same as Embodiment 1 and involves symbolshaving the same meanings as Embodiment 1, and only differencestherebetween will be described in the following.

Table 13 and Table 14 show design data of a camera optical lens 40 inEmbodiment 2 of the present disclosure.

TABLE 13 R d nd νd S1 ∞ d0= −0.587 R1 1.444 d1= 0.635 nd1 1.5264 ν176.86 R2 2.657 d2= 0.054 R3 2.974 d3= 0.501 nd2 1.5444 ν2 55.82 R442.181 d4= 0.119 R5 −21.008 d5= 0.230 nd3 1.6610 ν3 20.53 R6 5.049 d6=0.183 R7 4.071 d7= 0.230 nd4 1.5444 ν4 55.82 R8 1.999 d8= 1.199 R9−13.184 d9= 0.384 nd5 1.6610 ν5 20.53 R10 −7.012 d10= 0.910 R11 −3.064d11= 0.523 nd6 1.5346 ν6 55.69 R12 −11.923 d12= 0.392 R13 ∞ d13= 0.200ndg 1.5168 ν 64.17 R14 ∞ d14= 0.125

Table 14 shows aspheric surface data of respective lenses in the cameraoptical lens 40 according to Embodiment 4 of the present disclosure.

TABLE 14 Conic coefficient Aspherical surface coefficients k A4 A6 A8A10 A12 A14 A16 R1 −5.8735E−01 −1.5951E−02  6.4758E−02 −8.7183E−02  5.9710E−02 −7.7619E−03 −3.4104E−03 −7.9388E−04 R2 −5.2936E+01−1.8752E−01  2.7010E−01 −8.0383E−03   5.7828E−02 −1.6346E−02 −1.0757E−01 4.9020E−02 R3 −8.3033E+01 −1.6198E−01  2.1493E−01 2.4395E−01−1.6458E−01 −1.2721E−01  1.1959E−01 −2.9456E−02 R4  8.8973E+01−2.0238E−02  1.5785E−01 −1.7113E−01  −8.4836E−02  1.9489E−01 −5.0174E−02−2.0048E−02 R5 −9.9500E+02  6.2389E−02 −1.4119E−01 1.6484E−01 1.8893E−01 −6.2864E−01  6.4765E−01 −2.5149E−01 R6 −4.6000E+02 3.1586E−01 −1.1649E+00 2.6461E+00 −1.1127E+00 −5.1329E+00  9.9085E+00−5.4617E+00 R7  1.8948E+01 −3.4110E−01 −4.4705E−02 1.1232E+00−2.6819E+00  3.2308E+00 −1.6878E+00 −1.1472E−01 R8 −1.8355E+01 4.2511E−02 −1.2228E−01 2.1305E−01  2.1502E−01 −9.5578E−01  8.8608E−01−2.7433E−01 R9 −9.0001E+01 −6.9990E−02 −3.0235E−02 3.0813E−02−1.6014E−02 −2.1742E−03  4.7677E−03 −9.0683E−04 R10  1.6295E+01−6.0434E−02 −4.7513E−03 1.7077E−03  3.5338E−03 −3.7098E−03  1.0362E−03 2.5211E−05 R11 −1.7823E−01 −9.8986E−02  5.7568E−02 −1.0346E−02 −4.8599E−04  4.0287E−04 −3.8937E−05  4.8772E−07 R12 −5.5528E+02−1.6739E−01  7.8183E−02 −1.7154E−02   7.6111E−04  4.3973E−04 −9.6817E−05 6.5975E−06

Table 15 and Table 16 show design data of inflexion points and arrestpoints of respective lens in the camera optical lens 40 according toEmbodiment 4 of the present disclosure.

TABLE 15 Number of Inflexion point Inflexion point Inflexion pointinflexion points position 1 position 2 position 3 P1R1 1 1.175 P1R2 30.345 0.485 1.025 P2R1 3 0.335 0.435 1.055 P2R2 1 0.745 P3R1 2 0.2850.945 P3R2 P4R1 1 0.275 P4R2 1 0.785 P5R1 1 1.295 P5R2 1 1.415 P6R1 11.385 P6R2 1 2.205

TABLE 16 Number of Arrest point arrest points position 1 P1R1 P1R2 P2R1P2R2 1 0.985 P3R1 1 0.545 P3R2 P4R1 1 0.505 P4R2 P5R1 P5R2 P6R1 P6R2

FIG. 14 and FIG. 15 illustrate a longitudinal aberration and a lateralcolor of light with wavelengths of 470 nm, 510 nm, 555 nm, 610 nm and650 nm after passing the camera optical lens 40 according to Embodiment4. FIG. 16 illustrates a field curvature and a distortion of light witha wavelength of 555 nm after passing the camera optical lens 40according to Embodiment 4.

As shown in Table 17, Embodiment 4 satisfies respective conditions.

In this embodiment, the entrance pupil diameter of the camera opticallens is 2.479 mm. The image height of 1.0H is 2.629 mm. The FOV (fieldof view) is 45.11°. Thus, the camera optical lens is ultra-thin whileachieving a high optical performance.

TABLE 17 Embodi- Embodi- Embodi- Embodi- ment 1 ment 2 ment 3 ment 4Notes d1/d2 10.49 8.00 8.08 11.76 Condition (1) v1/v3 3.74 3.98 2.893.74 Condition (2) f5/f1 3.93 3.15 4.95 4.32 Condition (3) (R3 + R4)/−2.58 −4.66 −4.98 −1.15 Condition (R3 − R4) (4) f1/f 0.61 0.56 0.51 0.79Condition (5) (R7 + R8)/ 1.67 1.01 1.05 2.93 Condition (R7 − R8) (6) f6.445 6.445 6.445 6.444 f1 3.906 3.622 3.276 5.077 f2 11.319 22.48229.850 5.831 f3 −6.447 −7.231 −6.223 −6.084 f4 −6.179 −5.569 −7.612−7.484 f5 15.348 11.409 16.218 21.921 f6 −8.258 −7.801 −6.544 −7.849 f122.960 3.105 2.922 2.929

It can be appreciated by one having ordinary skill in the art that thedescription above is only embodiments of the present disclosure. Inpractice, one having ordinary skill in the art can make variousmodifications to these embodiments in forms and details withoutdeparting from the spirit and scope of the present disclosure

What is claimed is:
 1. A camera optical lens, comprising, from an objectside to an image side: an aperture; a first lens having a positiverefractive power; a second lens having a positive refractive power; athird lens having a negative refractive power; a fourth lens having anegative refractive power; a fifth lens having a positive refractivepower; and a sixth lens having a negative refractive power, wherein thecamera optical lens satisfies following conditions:8.00≤d1/d2≤12.00; and2.80≤v1/v3≤4.00, where d1 denotes an on-axis thickness of the firstlens; d2 denotes an on-axis distance from an image side surface of thefirst lens to an object side surface of the second lens; v1 denotes anabbe number of the first lens; and v3 denotes an abbe number of thethird lens.
 2. The camera optical lens as described in claim 1, furthersatisfying a following condition:3.00≤f5/f1≤5.00, where f1 denotes a focal length of the first lens; andf5 denotes a focal length of the fifth lens.
 3. The camera optical lensas described in claim 1, further satisfying a following condition:−5.00≤(R3+R4)/(R3−R4)≤−1.00, where R3 denotes a curvature radius of theobject side surface of the second lens; and R4 denotes a curvatureradius of an image side surface of the second lens.
 4. The cameraoptical lens as described in claim 1, further satisfying a followingcondition:0.50≤f1/f≤0.80, where f denotes a focal length of the camera opticallens; and f1 denotes a focal length of the first lens.
 5. The cameraoptical lens as described in claim 1, further satisfying a followingcondition:1.00≤(R7+R8)/(R7−R8)≤3.00, where R7 denotes a curvature radius of anobject side surface of the fourth lens; and R8 denotes a curvatureradius of an image side surface of the fourth lens.